Undergrad Minkowski metric and proper time interpretation

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The discussion centers on the interpretation of the Minkowski metric in the context of general relativity, specifically regarding how time is affected by gravity. It is clarified that a clock ticks slower near a heavy mass, and the proper time, represented by dτ, is indeed what is measured by a clock in a gravitational field. The confusion arises from the misunderstanding of the parameter 'a' in the metric, which should be less than 1 for the Schwarzschild metric. The local nature of the metric is emphasized, indicating that comparisons should be made with a reference clock at y=0, rather than at infinity. Ultimately, the participants reach a clearer understanding of how gravitational effects influence time measurement in different locations.
msumm21
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I'm trying to learn general relativity, but misunderstanding how the metric implies that time appears to pass slower for something near a heavy mass, as viewed from something far away
Using an example of 1 space dimension and 1 time dimension, consider the metric ##d\tau^2 = a dt^2 - dx^2## near a heavy mass (##a>1##).

From what I've read a clock ticks slower near a heavy mass, as viewed from an observer far away. A clock tick would be representative of ##d\tau## right (not ##dt##)? If so, then my confused understanding is below.

If ##a## is large, then small ##dt## results in large ##d\tau##. If the far away observer's ##d\tau## is approximately ##dt##, then his clock tick, say ##dt=1## corresponds to ##d\tau >> 1## near the mass. My interpretation of this is that the clock near the mass ticks ##d\tau >> dt## ticks (it ticks more than the clock far from the mass), and hence the clock near the mass moves faster. I realize this is wrong, but not clear what part is wrong.
 
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Your basic assumption is wrong: ##a < 1## for the Schwarzschild metric.
 
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The book I'm reading (General Relativity: The Theoretical Minimum by Susskind) says the metric is approximately ##d\tau^2 = (1+2gy)dt^2 - dy^2## where the grav potential is ##gy## but yes I see this doesn't jive with stuff I see on Wikipedia. I must have misunderstood what this metric was supposed to be in the first place. Does anyone know what this metric is?
 
msumm21 said:
I must have misunderstood what this metric was supposed to be in the first place. Does anyone know what this metric is?
This is a local metric, only valid in a small region. The reference is not a clock at infinity, but a clock at ##y=0##. Clocks at higher ##y## will be faster and clocks at lower ##y## will be slower compared to the reference clock.
 
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Dale said:
This is a local metric, only valid in a small region. The reference is not a clock at infinity, but a clock at y=0. Clocks at higher y will be faster and clocks at lower y will be slower compared to the reference clock.
Oh yes I think I'm getting it now, thanks!
 
Moderator's note: Spin-off from another thread due to topic change. In the second link referenced, there is a claim about a physical interpretation of frame field. Consider a family of observers whose worldlines fill a region of spacetime. Each of them carries a clock and a set of mutually orthogonal rulers. Each observer points in the (timelike) direction defined by its worldline's tangent at any given event along it. What about the rulers each of them carries ? My interpretation: each...

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